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A magnetostatic energy formula arising from the L-2-orthogonal decomposition of the stray field

机译:由杂散场的L-2 - 正交分解产生的磁静电能公式

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A formula for the magnetostatic energy of a finite magnet is proven. In contrast to common approaches, the new energy identity does not rely on evaluation of a nonlocal boundary integral inside the magnet or the solution of an equivalent Dirichlet problem. The formula is therefore computationally efficient, which is also shown numerically. Algorithms for the simulation of magnetic materials could benefit from incorporating the presented representation of the energy. In addition, a natural analogue for the energy via the magnetic induction is given. Proofs are carried out within a setting which is suitable for common discretizations in computational micromagnetics. (C) 2018 Elsevier Inc. All rights reserved.
机译:已证明有限磁体的磁化能量的公式。 与常见方法相比,新能量标识不依赖于评估磁铁内部的非局部边界或等同的Dirichlet问题的溶液。 因此,该公式是计算有效的,其也是在数值上示出的。 用于仿真磁性材料的算法可以从结合所呈现的能量表示中受益。 另外,给出了通过磁感应的能量的自然类似物。 在适用于计算微磁中的常见离散化的设置内进行证明。 (c)2018 Elsevier Inc.保留所有权利。

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